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Diffusion within α-CuI studied using ab initio molecular dynamics simulations

机译:使用从头算分子动力学模拟研究α-CuI中的扩散

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The structure and dynamics of superionic α-CuI are studied in detail by means of ab initio Born_Oppenheimer molecular dynamics simulations. The extreme cation disorder and a soft immobile face centred cubic sublattice are evident from the highly diffuse atomic density profiles. The Cu-Cu pair distribution function and distribution of Cu-I-Cu bond angles possess distinct peaks at 2.6 _ and 60° respectively, which are markedly lower than the values expected from the average cationic density, pointing to the presence of pronounced short-range copper_copper correlations. Comparison with lattice static calculations shows that these correlations and the marked shift in the cationic density profile in the (111) directions are associated with a locally distorted cation sublattice, and that the movements within the tetrahedral cavities involve rapid jumps into and out of shallow basins on the system potential energy surface. On average, the iodines are surrounded by three coppers within their first coordination shell, with the fourth copper being located in a transition zone between two neighbouring iodine cavities. However, time-resolved analysis reveals that the local structure actually involves a mixture of threefold-, fourfold- and fivefold-coordinated iodines. Examination of the ionic trajectories shows that the copper ions jump rapidly to nearest neighbouring tetrahedral cavities (aligned in the (100) directions) following a markedly curved trajectory and often involving short-lived (( )1 ps) interstitial positions. The nature of the correlated diffusion underlying the unusually high fraction of coppers with short residence time can be attributed to the presence of a large number of `unsuccessful' jumps and the likelihood of cooperative motion of pairs of coppers. The calculated diffusion coefficient at 750 K, D~(Cu) = 2.8 × 10~(-5) cm~2 s~(-1), is in excellent agreement with that found experimentally.
机译:通过从头开始的Born_Oppenheimer分子动力学模拟,详细研究了超离子α-CuI的结构和动力学。从高度扩散的原子密度分布图可以看出,极端的阳离子紊乱和不动的,以面为中心的立方亚晶格很明显。 Cu-Cu对分布函数和Cu-I-Cu键角分布分别在2.6_和60°处具有明显的峰,这些峰明显低于平均阳离子密度所预期的值,表明存在明显的短峰。范围copper_copper相关。与晶格静态计算的比较表明,这些相关性和在(111)方向上阳离子密度分布的明显偏移与局部变形的阳离子亚晶格有关,并且四面体腔内的运动涉及到浅盆地的快速跳入和跳出。在系统势能面上。平均而言,碘在它们的第一个配位壳内被三个铜包围,而第四个铜位于两个相邻的碘腔之间的过渡区。但是,时间分辨分析表明,局部结构实际上涉及三倍,四倍和五倍协调的碘的混合物。离子轨迹的检查表明,铜离子沿明显弯曲的轨迹迅速跳至最近的相邻四面体腔(沿(100)方向排列),并且经常涉及短命(()1 ps)间隙位置。具有短停留时间的异常高比例的铜所引起的相关扩散的性质可以归因于大量“不成功”跳跃的存在以及成对的铜协同运动的可能性。在750 K,D〜(Cu)= 2.8×10〜(-5)cm〜2 s〜(-1)时计算出的扩散系数与实验结果非常吻合。

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